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格子玻尔兹曼方法对具有弯曲无滑移壁面的流体流动边界条件的离散效应。

Discrete effects on boundary conditions of the lattice Boltzmann method for fluid flows with curved no-slip walls.

作者信息

Wang Liang, Tao Shi, Meng Xuhui, Zhang Kai, Lu Gui

机构信息

Beijing Key Laboratory of Emission Surveillance and Control for Thermal Power Generation, North China Electric Power University, Beijing 102206, China.

School of Energy Power and Mechanical Engineering, North China Electric Power University, Beijing 102206, China.

出版信息

Phys Rev E. 2020 Jun;101(6-1):063307. doi: 10.1103/PhysRevE.101.063307.

Abstract

The lattice Boltzmann method (LBM) has been formulated as a powerful numerical tool to simulate incompressible fluid flows. However, it is still a critical issue for the LBM to overcome the discrete effects on boundary conditions successfully for curved no-slip walls. In this paper, we focus on the discrete effects of curved boundary conditions within the framework of the multiple-relaxation-time (MRT) model. We analyze in detail a single-node curved boundary condition [Zhao et al., Multiscale Model. Simul. 17, 854 (2019)10.1137/18M1201986] for predicting the Poiseuille flow and derive the numerical slip at the boundary dependent on a free parameter as well as the distance ratio and the relaxation times. An approach by virtue of the free parameter is then proposed to eliminate the slip velocity while with uniform relaxation parameters. The theoretical analysis also indicates that for previous curved boundary schemes only with the distance ratio and the halfway bounce-back (HBB) boundary scheme, the numerical slip cannot be removed with uniform relaxation times virtually. We further carried out some simulations to validate our theoretical derivations, and the numerical results for the case of straight and curved boundaries confirm our theoretical analysis. Finally, for fluid flows with curved boundary geometries, resorting to more degrees of freedom from the boundary scheme may have more potential to eliminate the discrete effect at the boundary with uniform relaxation times.

摘要

格子玻尔兹曼方法(LBM)已被确立为模拟不可压缩流体流动的一种强大数值工具。然而,对于LBM而言,要成功克服弯曲无滑移壁面边界条件下的离散效应仍是一个关键问题。在本文中,我们聚焦于多松弛时间(MRT)模型框架内弯曲边界条件的离散效应。我们详细分析了一种用于预测泊肃叶流动的单节点弯曲边界条件[Zhao等人,《多尺度模型与模拟》17, 854 (2019)10.1137/18M1201986],并推导出边界处的数值滑移,其取决于一个自由参数以及距离比和松弛时间。随后提出了一种借助自由参数的方法,以在松弛参数均匀的情况下消除滑移速度。理论分析还表明,对于仅具有距离比的先前弯曲边界方案以及中途反弹(HBB)边界方案,实际上无法在松弛时间均匀的情况下消除数值滑移。我们进一步进行了一些模拟以验证我们的理论推导,直边界和曲边界情况的数值结果证实了我们的理论分析。最后,对于具有弯曲边界几何形状的流体流动,借助边界方案中更多的自由度可能更有潜力在松弛时间均匀的情况下消除边界处的离散效应。

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